Table C.1.
Photometric upper limits in multiple bands computed from our X-shooter spectra.
Object | B | V | G | R | I | Y | J | H | Ks |
---|---|---|---|---|---|---|---|---|---|
S1 | 21.3 ± 0.4 | 20.8 ± 0.4 | 19.9 ± 0.3 | 19.7 ± 0.4 | 18.7 ± 0.5 | 18.6 ± 0.3 | 17.9 ± 0.2 | 16.8 ± 0.4 | 16.1 ± 0.3 |
S1-SE | 22.5 ± 0.7 | 21.4 ± 0.4 | 20.3 ± 0.3 | 20.1 ± 0.4 | 18.9 ± 0.5 | 18.6 ± 0.2 | 17.8 ± 0.2 | 16.6 ± 0.5 | 15.7 ± 0.3 |
S2 | – | – | – | – | – | – | 21.6 ± 3.4 | 17.9 ± 3.3 | 15.7 ± 0.4 |
S3 | – | – | 19.7 ± 0.5 | 19.0 ± 0.5 | 18.7 ± 0.6 | 18.9 ± 0.4 | 18.6 ± 0.4 | 17.4 ± 0.5 | 15.8 ± 0.5 |
S3-K | 20.4 ± 0.4 | 19.0 ± 0.3 | 17.4 ± 0.3 | 17.3 ± 0.3 | 15.7 ± 0.4 | 15.3 ± 0.3 | 15.0 ± 0.2 | 13.7 ± 0.3 | 13.2 ± 0.3 |
S4 | 19.1 ± 0.4 | 19.0 ± 0.4 | 18.2 ± 0.3 | 18.0 ± 0.4 | 17.1 ± 0.5 | 17.3 ± 0.3 | 16.7 ± 0.2 | 14.5 ± 0.3 | 12.7 ± 0.3 |
S5-A | 16.8 ± 0.4 | 16.6 ± 0.4 | 16.2 ± 0.4 | 15.9 ± 0.4 | 15.5 ± 0.4 | 16.1 ± 0.3 | 16.9 ± 0.2 | 16.4 ± 0.4 | 16.2 ± 0.3 |
S5-B | 19.1 ± 0.5 | 19.1 ± 0.4 | 18.7 ± 0.4 | 18.5 ± 0.5 | 18.2 ± 0.4 | 19.0 ± 0.3 | 19.9 ± 0.6 | 19.6 ± 2.4 | 18.9 ± 3.1 |
S5-C | 18.3 ± 0.4 | 18.4 ± 0.4 | 18.2 ± 0.6 | 18.4 ± 0.5 | 18.1 ± 0.4 | 19.0 ± 0.3 | 20.1 ± 0.6 | 19.7 ± 3.1 | 20.5 ± 5.1 |
S5-D | 20.6 ± 0.6 | 20.0 ± 0.4 | 19.1 ± 0.3 | 18.7 ± 0.4 | 17.9 ± 0.4 | 18.3 ± 0.3 | 18.3 ± 0.3 | 17.2 ± 3.9 | 17.3 ± 0.5 |
S5-E | 20.6 ± 0.6 | 19.8 ± 0.5 | 19.5 ± 0.6 | 19.0 ± 0.6 | 19.3 ± 0.4 | 19.4 ± 0.3 | 20.0 ± 0.5 | 18.0 ± 0.4 | 15.0 ± 0.3 |
S5-F | 17.8 ± 0.4 | 17.6 ± 0.5 | 17.5 ± 0.6 | 17.7 ± 0.4 | 17.2 ± 0.6 | 18.1 ± 0.4 | 19.4 ± 0.5 | 18.9 ± 2.5 | 17.4 ± 0.8 |
S6 | – | 17.9 ± 0.7 | 18.1 ± 1.1 | – | 20.2 ± 1.0 | 18.4 ± 0.4 | 17.2 ± 0.2 | 14.8 ± 0.5 | 13.2 ± 0.3 |
S7-A | 17.9 ± 0.4 | 17.8 ± 0.4 | 17.5 ± 0.4 | 17.4 ± 0.5 | 17.2 ± 0.5 | 17.5 ± 0.3 | 16.6 ± 0.2 | 14.8 ± 0.3 | 13.2 ± 0.3 |
S7-B | 19.7 ± 0.4 | 19.2 ± 0.4 | 18.7 ± 0.3 | 18.4 ± 0.4 | 17.8 ± 0.6 | 18.6 ± 0.6 | 17.7 ± 0.2 | 15.3 ± 0.3 | 13.1 ± 0.3 |
S8 | 21.9 ± 0.5 | 20.8 ± 0.4 | 19.5 ± 0.3 | 19.4 ± 0.4 | 18.0 ± 0.5 | 17.8 ± 0.3 | 17.6 ± 0.3 | 16.2 ± 0.5 | 14.9 ± 0.4 |
S9 | – | 21.1 ± 0.5 | 20.9 ± 0.5 | 20.8 ± 0.5 | 20.0 ± 0.6 | 20.1 ± 0.6 | 19.8 ± 0.8 | 17.4 ± 2.3 | 15.6 ± 3.7 |
S10-A | – | 21.1 ± 0.5 | 20.9 ± 0.5 | 21.0 ± 0.6 | 20.0 ± 0.7 | 20.9 ± 1.3 | 20.8 ± 1.8 | – | 16.2 ± 0.5 |
S10-BC | – | 21.0 ± 0.5 | 20.8 ± 0.5 | 20.6 ± 0.6 | 20.0 ± 0.6 | 20.4 ± 0.7 | 20.0 ± 0.7 | 18.0 ± 0.6 | 16.4 ± 0.4 |
S10-K | – | 21.1 ± 0.6 | 21.1 ± 0.7 | 21.2 ± 1.2 | 20.5 ± 0.7 | 21.5 ± 2.9 | 20.2 ± 0.8 | 17.5 ± 2.8 | 15.8 ± 0.4 |
S10-SW-A | 22.4 ± 0.7 | 21.2 ± 0.4 | 20.1 ± 0.4 | 19.7 ± 0.4 | 18.8 ± 0.6 | 18.6 ± 0.3 | 17.7 ± 0.2 | 16.1 ± 0.5 | 14.7 ± 0.3 |
S10-SW-B | – | 22.3 ± 0.8 | 22.4 ± 1.2 | 22.8 ± 2.4 | 23.3 ± 6.7 | 21.0 ± 1.3 | 19.7 ± 0.4 | 17.9 ± 0.4 | 16.6 ± 0.4 |
R135 | 13.5 ± 0.5 | 13.7 ± 0.4 | 13.2 ± 0.5 | 12.9 ± 0.5 | 12.9 ± 0.4 | 13.4 ± 0.2 | 13.4 ± 0.2 | 13.2 ± 0.3 | 13.1 ± 0.3 |
Notes. All magnitudes are upper limits computed using Eq. (1). For the B, V, R, and I-bands we used the Bessell photometric system (Bessell 1990), for the G-band we used the Gaia photometric system (Gaia Collaboration 2016), and for the Y, J, H and Ks-bands we used the VISTA photometric system. The empty band values resulted from a negative integrated flux in the corresponding band. The objects shown in bold are the MYSOs confirmed in this work.
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.